Timeline for $\gamma$ in Newton's Second Law of Motion in Differential Form
Current License: CC BY-SA 3.0
10 events
| when toggle format | what | by | license | comment | |
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| S Oct 9, 2013 at 14:01 | history | edited | Emilio Pisanty | CC BY-SA 3.0 |
Improved wording
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| S Oct 9, 2013 at 14:01 | history | suggested | Alenanno | CC BY-SA 3.0 |
Improved wording
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| Oct 9, 2013 at 14:00 | review | Suggested edits | |||
| Oct 9, 2013 at 14:01 | |||||
| Oct 3, 2013 at 12:00 | vote | accept | user93089 | ||
| Oct 3, 2013 at 11:53 | answer | added | xuanji | timeline score: 3 | |
| Oct 3, 2013 at 10:25 | history | edited | Qmechanic♦ |
edited tags
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| Oct 3, 2013 at 10:18 | comment | added | Qmechanic♦ | Comment to the question (v1): A force of the type $\vec{F}=-\gamma \vec{v}$ is known as kinetic friction, damping, or Stokes' drag, depending on the context. | |
| Oct 3, 2013 at 9:54 | answer | added | MoonKnight | timeline score: 0 | |
| Oct 3, 2013 at 9:52 | comment | added | Ruslan | Looks like it has something to do with viscosity. | |
| Oct 3, 2013 at 9:43 | history | asked | user93089 | CC BY-SA 3.0 |